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Dear student,
We consider a Gaussian surface of a pill box extremely small length and extremely small cross-section as σ.
A fraction of it ls inside the surface and tht remaining part is outside the surface.
The total charge enclosed by this pill box is q =σ ds
where σ = surface charge density of conductor.
At every point on the surface of the conductor E is perpendicular to the surface. Hence, it is parallel to the surface vector E∣∣ds
But inside the surface E=0 .
Hence, the flux coming out from the cross-section of pill box inside the surface=0
The flux coming out from the cross-section of pill box outside the surface,
Regards
We consider a Gaussian surface of a pill box extremely small length and extremely small cross-section as σ.
A fraction of it ls inside the surface and tht remaining part is outside the surface.
The total charge enclosed by this pill box is q =σ ds
where σ = surface charge density of conductor.
At every point on the surface of the conductor E is perpendicular to the surface. Hence, it is parallel to the surface vector E∣∣ds
But inside the surface E=0 .
Hence, the flux coming out from the cross-section of pill box inside the surface=0
The flux coming out from the cross-section of pill box outside the surface,
Regards